Method and apparatus for drug product tracking using encoded optical identification elements

ABSTRACT

A method and apparatus for drug product tracking (or other pharmaceutical, health care or cosmetics products, and/or the packages or containers they are supplied with) using diffraction grating-based encoded optical identification elements  8  includes an optical substrate  10  having at least one diffraction grating  12  disposed therein. The grating  12  has one or more colocated pitches Λ which represent a unique identification digital code that is detected when illuminated by incident light  24 . The incident light  24  may be directed transversely from the side of the substrate  10  (or from an end) with a narrow band (single wavelength) or multiple wavelength source, and the code is represented by a spatial distribution of light or a wavelength spectrum, respectively, or a combination thereof. The encoded element  8  may be used to label any desired item, such as drugs or medicines, or other pharmaceutical or health care products or cosmetics. The label may be used for many different purposes, such as for sorting, tracking, identification, verification, authentication, anti-theft/anti-counterfeit, security/anti-terrorism, or for other purposes. In a manufacturing environment, the elements  8  may be used to track inventory for production information or sales of goods/products. Such labeling provides product identification at the pill or liquid medicine level, which provides traceability of these products to their manufacturer, thereby reducing counterfeit products in the marketplace. Also, the elements  8  may be incorporated into a film, liquid, coating or adhesive tape at attached to the product package.

CROSS REFERENCES TO RELATED APPLICATIONS

This application claims the benefit of U.S. Provisional PatentApplications, Ser. Nos. 60/589,644 (CyVera Docket No. CV-0080PR), filedJul. 21, 2004; Ser. No. 60/609,712 (CyVera Docket No. CV-0084PR), filedSep. 13, 2004; Ser. No. 60/623,811 (CyVera Docket No. CV-0093PR), filedOct. 29, 2004; and is a continuation-in-part of U.S. patent applicationSer. No. 10/661,082, (CyVera Docket No. CV-0040), filed Sep. 12, 2003,which is a continuation-in-part of U.S. patent application Ser. No.10/645,689 (CyVera Docket No. CV-0038), filed Aug. 20, 2003, whichclaimed the benefit of US provisional applications, Ser. No. 60/405,087(CyVera Docket No. CV-0005PR/Prior CC-0429PR) filed Aug. 20, 2002 andSer. No. 60/410,541 (CyVera Docket No. CV-0012PR/Prior CC-0543 PR),filed Sep. 12, 2002; and which is a continuation-in-part of U.S. patentapplication Ser. No. 10/661,082 (CyVera Docket No. CV-0039), filed Aug.20, 2003, which claimed the benefit of US provisional applications, Ser.No. 60/405,087 (CyVera Docket No. CV-0005PR/Prior CC-0429PR) filed Aug.20, 2002 and Ser. No. 60/410,541 (CyVera Docket No. CV-0012PR/PriorCC-0543 PR), filed Sep. 12, 2002; and which claimed the benefit of Ser.No. 60/410,541 (CyVera Docket No. CV-0012PR/Prior CC-0543 PR), filedSep. 12, 2002; all of which are incorporated herein by reference intheir entirety.

The following cases contain subject matter related to that disclosedherein and are incorporated herein by reference in their entirety: U.S.patent application Ser. No. 10/661,234, filed Sep. 12, 2003, entitled“Diffraction Grating-Based Optical Identification Element”, (CyVeraDocket No. CV-0038A); U.S. patent application Ser. No. 10/661,031, filedSep. 12, 2003, entitled “Diffraction Grating-Based EncodedMicro-particles for Multiplexed Experiments”, (CyVera Docket No.CV-0039A); U.S. patent application Ser. No. 10/661,115, filed Sep. 12,2003, entitled “Assay Stick”, (CyVera Docket No. CV-0041); U.S. patentapplication Ser. No. 10/661,836, filed Sep. 12, 2003, entitled “Methodand Apparatus for Aligning Microbeads in order to Interrogate the Same”,(CyVera Docket No. CV-0042); U.S. patent application Ser. No.10/661,254, filed Sep. 12, 2003, entitled “Chemical Synthesis UsingDiffraction Grating-based Encoded Optical Elements”, (CyVera Docket No.CV-0043); U.S. patent application Ser. No. 10/661,116, filed Sep. 12,2003, entitled “Method of Manufacturing of a Diffraction grating-basedidentification Element”, (CyVera Docket No. CV-0044); and U.S. patentapplication Ser. No. 10/763,995 filed Jan. 22, 2004, entitled, “HybridRandom Bead/Chip Based Microarray”, (CyVera Docket No. CV-0054); andU.S. Provisional patent application, Serial No. (CyVera Docket Nos.CV-0092 PR), filed Oct. 1, 2004.

TECHNICAL FIELD

This invention relates to drug tracking, and more particularly to drugproduct tracking using encoded optical identification elements.

BACKGROUND ART

It is often desirable to uniquely label or identify items, such as largeor small objects, plants, and/or animals for sorting, tracking,identification, verification, authentication, or for other purposes.Existing technologies, such as bar codes, electronicmicrochips/transponders, radio-frequency identification (RFID), andfluorescence (or other optical techniques), are often inadequate. Forexample, existing technologies may be too large for certainapplications, may not provide enough different codes, cannot be madeflexible or bendable, or cannot withstand harsh environments, e.g.,harsh temperature, pressure, chemical, nuclear and/or electromagneticenvironments.

It is also been a problem in the pharmaceutical industry to havecounterfeit drugs be produced causing loss of security, traceability,and safety in the drug supply.

Therefore, it would be desirable to obtain a labeling technique thatprovides the capability of providing many codes (e.g., greater than 1million codes), that can be made very small, can be made flexible orbendable, and/or that can withstand harsh environments.

SUMMARY OF THE INVENTION

Objects of the present invention include provision of a labelingtechnique that allows for a large number of distinct codes, can be madevery small, can be made flexible or bendable, and/or can withstand harshenvironments.

According to a first aspect of the present invention, an opticalidentification element for identifying a drug, comprises an opticalsubstrate; at least a portion of the substrate having at least onediffraction grating disposed therein, the grating having at least onerefractive index pitch superimposed at a common location; the gratingproviding an output optical signal when illuminated by an incident lightsignal; the optical output signal being indicative of a code; and theelement being at least partially disposed on the drug or the packagingor containers associated therewith.

According to a second aspect of the present invention, a method ofreading a code in an optical identification element that is disposed ona drug, the element having a diffraction grating with one or morerefractive index pitches superimposed at a common location, comprises:illuminating the element with incident light, the substrate providing anoutput light signal; and reading the output light signal and detecting acode therefrom.

According further to the present invention, the element is at leastpartially embedded or attached to the drug or the packaging orcontainers associated therewith.

According further to the present inventions, said refractive indexvariation comprises at least one refractive index pitch superimposed atsaid grating location.

According still further to the present invention, said refractive indexvariation comprises a plurality of refractive index pitches superimposedat said grating location. According still further to the presentinvention, said substrate is made of a material selected from the group:glass, silica, plastic, rubber, and polymer.

The present invention provides a method and apparatus for labeling anitem, using diffraction grating-based encoded optical identificationelements, capable of having many optically readable codes. The elementhas a substrate containing an optically readable composite diffractiongrating having a one or more of collocated index spacing or pitches A.The invention allows for a high number of uniquely identifiable codes(e.g., millions, billions, or more). The codes may be digital binarycodes and thus are digitally readable or may be other numerical bases ifdesired.

The encoded element 8 may be used to label any desired item, such aslarge or small objects, products, solids, powders, liquids, gases,plants, minerals, cells and/or animals, or any combination of or portionof one or more thereof.

The elements 8 may be used on or within any consumer goods, lawenforcement applications, explosives, collectibles, sporting goods,forestry, textiles/apparel, firearms, documents, secure notes, bottles,blister packs, plastics, resins, films, adhesives, laminates, securitythreads, printing, paper, and/or polymers.

The label may be used for many different purposes, such as for sorting,tracking, identification, verification, authentication,anti-theft/anti-counterfeit, security/anti-terrorism, forensics, or forother purposes. In a manufacturing environment, the elements 8 may beused to track inventory for production information or sales ofgoods/products.

The element may be made of a glass material, such as silica or otherglasses, or may be made of plastic or polymer, or any other materialcapable of having a diffraction grating disposed therein. The elementmay be cylindrical in shape or any other geometry, provided the designparameters are met.

Also, the elements may be very small “microbeads” (or microelements ormicroparticles or encoded particles) for small applications (about1-1000 microns), or larger “macrobeads” (or macroelements) for largerapplications (e.g., 1-1000 mm or much larger). Also, the element may beembedded within or part of a larger substrate or object. The element mayalso be in the form of a thread or fiber or filaments to be weaved intoa material.

Also, the encoded element may be embedded in a film or coating, whichmay be an adhesive film or coating or tape, having one or a plurality ofparticles or filaments therein. For example a roll of encoded adhesivetape that may be easily attached to an item for labeling.

The code in the element is interrogated using free-space optics and canbe made alignment insensitive. The element may be optically interrogatedto read the code from the side or end of the element.

The gratings (or codes) are embedded inside (including on or near thesurface) of the substrate and may be permanent non-removable codes thatcan operate in harsh environments (chemical, temperature, pressure,nuclear, electromagnetic, etc.).

The code is not affected by spot imperfections, scratches, cracks orbreaks in the substrate. In addition, the codes are spatially invariant.Thus, splitting or slicing an element axially produces more elementswith the same code. Accordingly, when a bead is axially split-up, thecode is not lost, but instead replicated in each piece.

The foregoing and other objects, features and advantages of the presentinvention will become more apparent in light of the following detaileddescription of exemplary embodiments thereof.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a side view of an optical identification element, inaccordance with the present invention.

FIG. 2 is a top level optical schematic for reading a code in an opticalidentification element, in accordance with the present invention.

FIG. 3, illustrations (a)-(d) show various transparent items that can belabeled with an optical identification element, in accordance with thepresent invention.

FIG. 4, illustrations (a)-(c) show various integrated circuits orsilicon wafers, that can be labeled with an optical identificationelement, in accordance with the present invention.

FIG. 5 shows a cell or the like disposed on an optical identificationelement, in accordance with the present invention.

FIG. 6, illustrations (a)-(d) show fluids or powders that can be labeledwith an optical identification element, in accordance with the presentinvention.

FIG. 7, illustrations (a)-(v) show various other items that can belabeled with an optical identification element, in accordance with thepresent invention.

FIG. 8 shows a bit format for a code in an optical identificationelement, in accordance with the present invention.

FIG. 9 is an optical schematic for reading a code in an opticalidentification element, in accordance with the present invention.

FIG. 10 is an image of a code on a CCD camera from an opticalidentification element, in accordance with the present invention.

FIG. 11 is a graph showing a digital representation of bits in a code inan optical identification element, in accordance with the presentinvention.

FIG. 12 illustrations (a)-(c) show images of digital codes on a CCDcamera, in accordance with the present invention.

FIG. 13 illustrations (a)-(d) show graphs of different refractive indexpitches and a summation graph, in accordance with the present invention.

FIG. 14 is an alternative optical schematic for reading a code in anoptical identification element, in accordance with the presentinvention.

FIG. 15 illustrations (a)-(b) are graphs of reflection and transmissionwavelength spectrum for an optical identification element, in accordancewith the present invention.

FIGS. 16-17 are side views of a thin grating for an opticalidentification element, in accordance with the present invention.

FIG. 18 is a perspective view showing azimuthal multiplexing of a thingrating for an optical identification element, in accordance with thepresent invention.

FIG. 19 is side view of a blazed grating for an optical identificationelement, in accordance with the present invention.

FIG. 20 is a graph of a plurality of states for each bit in a code foran optical identification element, in accordance with the presentinvention.

FIG. 21 is a side view of an optical identification element where lightis incident on an end face, in accordance with the present invention.

FIGS. 22-23 are side views of an optical identification element wherelight is incident on an end face, in accordance with the presentinvention.

FIGS. 24, illustrations (a)-(c) are side views of an opticalidentification element having a blazed grating, in accordance with thepresent invention.

FIG. 25 is a side view of an optical identification element having acoating, in accordance with the present invention.

FIG. 26 is a side view of whole and partitioned optical identificationelement, in accordance with the present invention.

FIG. 27 is a side view of an optical identification element having agrating across an entire dimension, in accordance with the presentinvention.

FIG. 28, illustrations (a)-(c), are perspective views of alternativeembodiments for an optical identification element, in accordance withthe present invention.

FIG. 29, illustrations (a)-(b), are perspective views of an opticalidentification element having multiple grating locations, in accordancewith the present invention.

FIG. 30, is a perspective view of an alternative embodiment for anoptical identification element, in accordance with the presentinvention.

FIG. 31 is a view an optical identification element having a pluralityof gratings located rotationally around the optical identificationelement, in accordance with the present invention.

FIG. 32 illustrations (a)-(e) show various geometries of an opticalidentification element that may have holes therein, in accordance withthe present invention.

FIG. 33 illustrations (a)-(c) show various geometries of an opticalidentification element that may have teeth thereon, in accordance withthe present invention.

FIG. 34 illustrations (a)-(c) show various geometries of an opticalidentification element, in accordance with the present invention.

FIG. 35 is a side view an optical identification element having areflective coating thereon, in accordance with the present invention.

FIG. 36 illustrations (a)-(b) are side views of an opticalidentification element polarized along an electric or magnetic field, inaccordance with the present invention.

FIGS. 37-43 show various embodiments for using the present invention forlabeling drugs or packages associated therewith, in accordance with thepresent invention.

FIGS. 44-48 show various embodiments for using the present invention forlabeling, in accordance with the present invention.

FIGS. 49 and 50 show various embodiments for using the present inventionfor labeling an item, in accordance with the present invention.

FIGS. 51, 51A, 52, and 53 show various embodiments of encoded tape orfilm, in accordance with the present invention.

FIGS. 54-66 show various embodiments for reading encoded elements inreflection, in accordance with the present invention.

BEST MODE FOR CARRYING OUT THE INVENTION

Referring to FIG. 1, a diffraction grating-based optical identificationelement 8 (or encoded element or coded element) comprises a knownoptical substrate 10, having an optical diffraction grating 12 disposed(or written, impressed, embedded, imprinted, etched, grown, deposited orotherwise formed) in the volume of or on a surface of a substrate 10.The grating 12 is a periodic or aperiodic variation in the effectiverefractive index and/or effective optical absorption of at least aportion of the substrate 10.

The optical identification element described herein is the same as thatdescribed in Copending patent application Serial No. (CyVera Docket No.CV-0038A), publication number: WO 2004/025559; PCT/US 03/28874, which isincorporated herein by reference in its entirety.

In particular, the substrate 10 has an inner region 20 where the grating12 is located. The inner region 20 may be photosensitive to allow thewriting or impressing of the grating 12. The substrate 10 has an outerregion 18 which does not have the grating 12 therein.

The grating 12 is a combination of one or more individual spatialperiodic sinusoidal variations (or components) in the refractive indexthat are collocated at substantially the same location on the substrate10 along the length of the grating region 20, each having a spatialperiod (or pitch) A. The resultant combination of these individualpitches is the grating 12, comprising spatial periods (Λ1-Λn) eachrepresenting a bit in the code. Thus, the grating 12 represents a uniqueoptically readable code, made up of bits, where a bit corresponds to aunique pitch Λ within the grating 12. Accordingly, for a digital binary(0-1) code, the code is determined by which spatial periods (Λ1-Λn)exist (or do not exist) in a given composite grating 12. The code orbits may also be determined by additional parameters (or additionaldegrees of multiplexing), and other numerical bases for the code may beused, as discussed herein and/or in the aforementioned patentapplication.

The grating 12 may also be referred to herein as a composite orcollocated grating. Also, the grating 12 may be referred to as a“hologram”, as the grating 12 transforms, translates, or filters aninput optical signal to a predetermined desired optical output patternor signal.

The substrate 10 has an outer diameter D1 and comprises silica glass(SiO₂) having the appropriate chemical composition to allow the grating12 to be disposed therein or thereon. Other materials for the opticalsubstrate 10 may be used if desired. For example, the substrate 10 maybe made of any glass, e.g., silica, phosphate glass, borosilicate glass,or other glasses, or made of glass and plastic, or solely plastic. Forhigh temperature or harsh chemical applications, the optical substrate10 made of a glass material is desirable. If a flexible substrate isneeded, plastic, rubber or polymer-based substrate may be used. Theoptical substrate 10 may be any material capable of having the grating12 disposed in the grating region 20 and that allows light to passthrough it to allow the code to be optically read.

The optical substrate 10 with the grating 12 has a length L and an outerdiameter D1, and the inner region 20 diameter D. The length L can rangefrom very small “microbeads” (or microelements, micro-particles, orencoded particles), about 1-1000 microns or smaller, to larger“macroelements” for larger applications (about 1.0-1000 mm or greater).In addition, the outer dimension D1 can range from small (less than 1000microns) to large (1.0-1000 mm and greater). Other dimensions andlengths for the substrate 10 and the grating 12 may be used.

The optical substrate 10 with the grating 12 has a length L and an outerdiameter D1, and the inner region 20 diameter D. The length L can rangefrom very small (about 1-1000 microns or smaller) to large (about1.0-1000 mm or greater). In addition, the outer dimension D1 can rangefrom small (less than 1000 microns) to large (1.0-1000 mm and greater).Other dimensions and lengths for the substrate 10 and the grating 12 maybe used. Also, the element may be embedded within or part of a largersubstrate or object. The element may also be in the form of a thread orfiber to be weaved into a material.

The grating 12 may have a length Lg of about the length L of thesubstrate 10. Alternatively, the length Lg of the grating 12 may beshorter than the total length L of the substrate 10, as shown in FIG.11.

The outer region 18 is made of pure silica (SiO₂) and has a refractiveindex n2 of about 1.458 (at a wavelength of about 1553 nm), and theinner grating region 20 of the substrate 10 has dopants, such asgermanium and/or boron, to provide a refractive index n1 of about 1.453,which is less than that of outer region 18 by about 0.005. Other indicesof refraction n1,n2 for the grating region 20 and the outer region 18,respectively, may be used, if desired, provided the grating 12 can beimpressed in the desired grating region 20. For example, the gratingregion 20 may have an index of refraction that is larger than that ofthe outer region 18 or grating region 20 may have the same index ofrefraction as the outer region 18 if desired.

Referring to FIG. 2, an incident light 24 of a wavelength λ, e.g., 532nm from a known frequency doubled Nd:YAG laser or about 632 nm from aknown Helium-Neon laser, is incident on the grating 12 in the substrate10. Any other input wavelength λ can be used if desired provided λ iswithin the optical transmission range of the substrate (discussed moreherein and/or in the aforementioned patent application). A portion ofthe input light 24 passes straight through the grating 12, as indicatedby a line 25. The remainder of the input light 24 is reflected by thegrating 12, as indicated by a line 27 and provided to a detector 29. Theoutput light 27 may be a plurality of beams, each having the samewavelength λ as the input wavelength λ and each having a differentoutput angle indicative of the pitches (Λ1-Λn) existing in the grating12. Alternatively, the input light 24 may be a plurality of wavelengthsand the output light 27 may have a plurality of wavelengths indicativeof the pitches (Λ1-Λn) existing in the grating 12. Alternatively, theoutput light may be a combination of wavelengths and output angles. Theabove techniques are discussed in more detail herein and/or in theaforementioned patent application.

The detector 29 has the necessary optics, electronics, software and/orfirmware to perform the functions described herein. In particular, thedetector reads the optical signal 27 diffracted or reflected from thegrating 12 and determines the code based on the pitches present or theoptical pattern, as discussed more herein or in the aforementionedpatent application. An output signal indicative of the code is providedon a line 31.

The encoded element 8 may be used to label any desired item, such aslarge or small objects, products, solids, powders, liquids, gases,plants, minerals, and/or animals, or any combination of one or morethereof. The label may be used for many different purposes, such as forsorting, tracking, identification, verification, authentication,anti-theft/anti-counterfeit, security/anti-terrorism, forensics, or forother purposes. In a manufacturing environment, the elements 8 may beused to track inventory for production information or sales ofgoods/products.

For any of the labeled items described herein, the encoded elements 8may be tiny discrete microbeads (1 to 1000 microns long) embedded intothe surface of the item or the encoded element 8 may be a long strand ofglass or plastic fiber that is woven, inserted, impressed, or injectedinto the item being labeled. Alternatively, in the appropriate cases,the diffraction grating 12 may be written or impressed directly into thematerial, as discussed herein. In any case, the properties of theencoded element 8 do not change. For labeled items that are pliable,bendable, or flexible, the element 8 may be made of a bendable material,such as a polymer or plastic. Also, if the item material is soft orcompliant the beads may be pressed, pushed, hammered or shot into thematerial, either for side reading or end reading, depending on theapplication.

For any of the embodiments herein, the label on the item can be detectedby scanning the item with incident light and detecting the reflectedlight as discussed herein and/or in the aforementioned patentapplication. When an element 8 is embedded or attached to an item thatis not reflective or transparent to the incident light 24 and reflectedlight 27, and if the element 8 is not reflective, it may be desirable toilluminate the element from an axial end 8 to achieve best results forcode reading.

In general, the encoded elements 8 may be used to label any products orcomponents within a product and may be used for productmanufacturing/production identification.

Referring to FIG. 3, illustrations (a)-(d), encoded elements 8 may beused to label glass or plastic items, such as microscope slides 811,test tubes 813, beakers 815, cookware 817, storage containers and/orcovers, multi-well plates, micro-well plates, plastic bags, windshields,windows, glasses, contact lenses, other lenses, optical components,tape, bottles, displays, display cases, watch faces, mirrors, sample orpietri dishes, or any other item made of a material that is transparentor substantially transparent to the incident light 24 and reflectedlight 27 used for read the code in the encoded elements 8. The inventionmay be used to identify such glass or plastic items by writing thediffraction grating 12 directly into the material or by embedding intoor otherwise attaching the encoded elements 8 to the item. In the casewhere the code is written directly into the material, the material musthave sufficient photosensitivity to allow the diffraction grating 12 tobe written into the material with sufficient strength so the code can beoptically read. We have found that borosilicate glass has sufficientphotosensitivity to support the creation of a diffraction grating 12therein. Other glasses may be used.

Referring to FIG. 4, illustrations (a) and (b), the encoded elements 8may be used to label micron size products, such as, microcircuitscomputer chips, integrated circuits (IC's), or other small products orportions thereof. Referring to FIG. 4, illustration (c), the elements 8may also be used to label silicon wafers 59 or small portions or regions57 thereof before being cut into small devices or microcircuits.

Referring to FIG. 5, the elements 8 may be used to label any single ormultiple cells 101 that are attached to or otherwise disposed on theelement 8. The cells 101 may include: molecules, particles, elements,compounds, organisms, atoms, chemicals, acids, bases, nucleic acids,chemical libraries, DNA, polynucleotides, oligomers, RNA, proteins,peptides, polymers, hydrocarbons, or other cells. The cells 101 may bealive or dead, organic or inorganic, and may be individual or groups orchains of cells and may change or mutate over time.

Referring to FIG. 6, illustrations, (a)-(d), the encoded elements 8 maybe used to label a liquid or liquid products located in a container 801or in an open or closed flowing pipe or conduit 803, 805 respectively.In that case, the elements 8 are mixed with the liquid. In addition, theelements 8 may also be used to label powders, such as powdereddetergent, dirt, pulverized coal, gunpowder, anthrax, or any otherpowders located in a container 807, or in an open or closed flowing pipeor conduit 803,805, respectively. Also, the elements 8 may be used tolabel or identify any combination of fluids (liquids and/or gases)and/or powders. Also, the elements 8 may be used to label gases, such asgases in containers or gases flowing in a pipe or conduit, or gaseousby-products of reactions, such as combustion exhaust or other exhaust.Also, the elements 8 may be used to label liquid particles or dropletsin gas, such as steam. The elements 8 may be used to track the flow of aliquid, powder, gas, etc. in an industrial plant to determine where theliquid is flowing or has flown.

The elements 8 may be removed from a fluid, powder and/or gas solutionor mixture other material by electro-magnetic attraction (if theelements are electro-magnetic), skimmed off the surface (if the elements8 are less dense than the solution, i.e., buoyant or semi-buoyant), orfrom settling to the bottom of a container (if the elements 8 are moredense than the solution), or by filtering the solution with a straineror filter.

The elements 8 can placed in a fluid or powder and the fluid or powderis used for labeling an item. For example, the elements 8 may be mixedwith paint (or other adhesive fluid) and sprayed on an item, such as acar or boat (see FIG. 7, illustrations (b) and (c)) or any other itemthat can be sprayed or painted. The same may be done with a dry powderthat is sprayed on a newly painted or otherwise adhesive surface, orwith an adhesive powder that is sprayed on a dry, or painted or adhesivesurface.

Referring to FIG. 7, illustrations (a), (b), (c), (f), (g), and (h), inparticular, the encoded elements 8 may be used to label large and/orvaluable items such as cases 841 (e.g., suitcases, briefcases, garmentbags, and the like), cars 831, boats 833, paintings 835, china 837,jewelry 839, and the like. Also, the elements 8 may be used as a way ofputting the vehicle identification number (VIN) or other similaridentification information in a hidden location and/or in many locationson an item that can only be read by the proper equipment. The elements 8can be used to label photographs.

Referring to FIG. 7, illustrations (d), (e), and (r), the encodedelements 8 may also be used to label currency 829, coins, bills, orcredit cards. Also, the elements 8 may be used an alternative oraddition to magnetic strips currently used on many types of cards 825,e.g., access cards, key cards, ID cards, debit cards, credit cards, andthe like. In addition, the elements 8 may be used as part of a key 827.

Referring to FIG. 7, illustration (i), the elements 8 may be used tolabel food containers 847 and the like.

Referring to FIG. 7, illustrations (j) and (l), the elements 8 may beused to label building materials 843, e.g., wood, pressboard, compositeboards (e.g., made of wood, plastic, and/or metal particles), sheetrock,wallboard, wallpaper, molding, tiles and the like or other buildingmaterials. Similarly, the elements 8 may be used to label furniture orother home or office furnishings 845.

Referring to FIG. 7, illustrations (m), (o), and (p), the encodedelements 8 may be used to label any animals 649, creatures,people/humans 855, and/or plants, or parts thereof 853. Such a labelcould be used in addition to or instead of fingerprints, retina scans,DNA or other identification techniques or labels.

Referring to FIG. 7, illustrations (n) and (q), the encoded elements 8may be used to label documents 857, books 851, and/or packages.

Referring to FIG. 7, illustrations (s) and (t), the encoded elements 8may be used to label weapons, ammunition, explosive devices, guns 819,artillery, bullets 821, mortar, grenades, missiles, torpedoes,projectiles, fireworks, bombs, spacecraft, aircraft, satellites, jetengines, submarines and tanks.

Referring to FIG. 7, illustration (u), the encoded elements 8 may beused to label clothing 823, garments, uniforms, linens, leather,footware, headgear, or textiles.

Referring to FIG. 7, illustration (v), the encoded elements 8 may beused to label storage media, such as compact discs and digital videodiscs (DVD's), or any other devices that uses light to read information,video or audio tapes tapes, disc drives, and the like.

Referring to FIG. 8, the code may be a simple code or may be a morecomplex code having many pieces of information located in the code. Inaddition, the code may have checks within the code to ensure the code isread correctly. It can be viewed as a serial digital message, word, orframe consisting of N bits.

In particular, there may be start and stop bits 869, 871, respectively.The start and stop bits may each take up more than one bit location ifdesired. In addition there may be an error check portion of the message,such as a check sum or CRC (cyclic redundancy check) having apredetermined number of bits, and a code section 873 having apredetermined number of bits. The error check portion ensures that thecode which is obtained from the bead is accurate. Accordingly, having alarge number of bits in the element 8 allows for greater statisticalaccuracy in the code readout and decreases the likelihood of providingan erroneous code. Accordingly, if a code cannot be read without anerror, no code will be provided, avoiding an erroneous result. Any knowntechniques for digital error checking for single or multi-bit errors maybe used.

The code section 873 may be broken up into one or more groups of bits,for example, three bit groups 863,865,867, each bit group containinginformation about the bead itself or the item attached to the bead orhow the bead is to be used, or other information. For example, the firstbit group 863 may contain information regarding “identifying numbers”,such as: lot number, quality control number, model number, serialnumber, inventory control number; the second bit group 865 may contain“type” information, such as: chemical or cell type, experiment type,item type, animal type; and the third bit group 867 may contain “date”information, such as: manufactured date, experiment date, creation date,initial tracking date. Any other bit groups, number of bit groups, orsize of bit groups may be used if desired. Also, additional error orfault checking can be used if desired.

In particular, for a product manufacturing application, the code mayhave the serial number, the lot number, date of manufacture, etc. orhave other information that identifies the item and/or information aboutthe item. For a chemical or assay application, the code may haveinformation about the chemical attached to the bead, the date and/ortime of creation of the chemical or experiment, or other information ofinterest.

Referring to FIG. 9, The reflected light 27, comprises a plurality ofbeams 26-36 that pass through a lens 37, which provides focused lightbeams 46-56, respectively, which are imaged onto a CCD camera 60. Thelens 37 and the camera 60, and any other necessary electronics or opticsfor performing the functions described herein, make up the reader 29.Instead of or in addition to the lens 37, other imaging optics may beused to provide the desired characteristics of the optical image/signalonto the camera 60 (e.g., spots, lines, circles, ovals, etc.), dependingon the shape of the substrate 10 and input optical signals. Also,instead of a CCD camera other devices may be used to read/capture theoutput light.

Referring to FIG. 10, the image on the CCD camera 60 is a series ofilluminated stripes indicating ones and zeros of a digital pattern orcode of the grating 12 in the element 8. Referring to FIG. 11, lines 68on a graph 70 are indicative of a digitized version of the image of FIG.10 as indicated in spatial periods (Λ1-Λn).

Each of the individual spatial periods (Λ1-Λn) in the grating 12 isslightly different, thus producing an array of N unique diffractionconditions (or diffraction angles) discussed more hereinafter. When theelement 8 is illuminated from the side, in the region of the grating 12,at an appropriate input angle, e.g., about 30 degrees, with a singleinput wavelength λ (monochromatic) source, the diffracted (or reflected)beams 26-36 are generated. Other input angles θi may be used if desired,depending on various design parameters as discussed herein and/or in theaforementioned patent application, and provided that a known diffractionequation (Eq. 1 below) is satisfied:sin(θ_(i))+sin(θ_(o))=mλ/Λ  Eq. 1where Eq. 0.1 is the diffraction (or reflection or scatter) relationshipbetween the input wavelength λ (in free space or vacuum), input incidentangle θi, output incident angle θo, and the spatial period Λ of thegrating 12. Further, m is the “order” of the reflection being observed.The value of m=1 or first order reflection is acceptable forillustrative purposes. Eq. 1 applies to light incident on outer surfacesof the substrate 10 that are parallel to the longitudinal axis of thegrating (or the k_(B) vector). It should be understood by those skilledin the art that because the angles θi,θo are defined outside thesubstrate 10 and because the refractive index n of the substrate 10 issubstantially a constant value throughout the substrate 10, therefractive index n does not appear in Eq. 1.

Thus, for a given input wavelength λ, grating spacing Λ, and incidentangle of the input light θi, the angle θo of the reflected output lightmay be determined. Solving Eq. 1 for θo and plugging in m=1, gives:θo=sin⁻¹(λ/Λ−sin(θi))  Eq. 2For example, for an input wavelength λ=532 nm, a grating spacing Λ=0.532microns (or 532 nm), and an input angle of incidence θi=30 degrees, theoutput angle of reflection will be θo=30 degrees. Alternatively, for aninput wavelength λ=632 nm, a grating spacing Λ=0.532 microns (or 532nm), and an input angle θi of 30 degrees, the output angle of reflectionθo will be at 43.47 degrees, or for an input angle θi=36.44 degrees, theoutput angle of reflection will be θo=36.44 degrees. Any input anglethat satisfies the design requirements discussed herein and/or in theaforementioned patent application may be used.

In addition, to have sufficient optical output power and signal to noiseratio, the output light 27 should fall within an acceptable portion ofthe Bragg envelope (or normalized reflection efficiency envelope) curve200, as indicated by points 204,206, also defined as a Bragg envelopeangle θB, as also discussed herein and/or in the aforementioned patentapplication. The curve 200 (for a planar slab geometry) may be definedas: $\begin{matrix}{{I\left( {{ki},{ko}} \right)} \approx {\lbrack{KD}\rbrack^{2}\sin\quad{c^{2}\left\lbrack \frac{\left( {{ki} - {ko}} \right)D}{2} \right\rbrack}}} & {{Eq}.\quad 3}\end{matrix}$where K=2πδn/λ, where, δn is the local refractive index modulationamplitude of the grating and λ is the input wavelength,sinc(x)=sin(x)/x, and the vectors k_(i)=2πcos(θ_(i))/λ and k_(o)=2πcos(θ_(o))/λ are the projections of the incident light and the output (orreflected) light, respectively, onto the line 203 normal to the axialdirection of the grating 12 (or the grating vector k_(B)), D is thethickness or depth of the grating 12 as measured along the line 203(normal to the axial direction of the grating 12). While Eq. 3 isspecific to a planar slab geometry, other grating geometries, such as acylinder (or other shapes) may be used and will exhibit a similar Braggenvelope response curve. We have found that a value for δn of about 10⁻⁴in the grating region of the substrate is acceptable; however, othervalues may be used if desired.

Rewriting Eq. 3 gives the reflection efficiency profile of the Braggenvelope as: $\begin{matrix}{{{I\left( {{ki},{ko}} \right)} \approx {\left\lbrack \frac{2{\pi \cdot \delta}\quad{n \cdot D}}{\lambda} \right\rbrack^{2}\left\lbrack \frac{{Sin}(x)}{x} \right\rbrack}^{2}}{{{where}\text{:}\quad x} = {{\left( {{ki} - {ko}} \right){D/2}} = {\left( {\pi\quad{D/\lambda}} \right)*\left( {{\cos\quad\theta\quad{\mathbb{i}}} - {\cos\quad\theta\quad o}} \right)}}}} & {{Eq}.\quad 4}\end{matrix}$

Thus, when the input angle θi is equal to the output (or reflected)angle θ0 (i.e., θi=θ_(o)), the reflection efficiency 1 (Eqs. 3 & 4) ismaximized, which is at the center or peak of the Bragg envelope. Whenθi=θo, the input light angle is referred to as the Bragg angle as isknown. The efficiency decreases for other input and output angles (i.e.,θi # θ_(o)), as defined by Eqs. 3 & 4. Thus, for maximum reflectionefficiency and thus output light power, for a given grating pitch Λ andinput wavelength, the angle θi of the input light 24 should be set sothat the angle θo of the reflected output light equals the input angleθi.

Also, as the thickness or diameter D of the grating decreases, the widthof the sin(x)/x function (and thus the width of the Bragg envelope)increases and, the coefficient to or amplitude of the sinc² (or(sin(x)/x)² function (and thus the efficiency level across the Braggenvelope) also increases, and vice versa. Further, as the wavelength λincreases, the half-width of the Bragg envelope as well as theefficiency level across the Bragg envelope both decrease. Thus, there isa trade-off between the brightness of an individual bit and the numberof bits available under the Bragg envelope. Ideally, δn should be madeas large as possible to maximize the brightness, which allows D to bemade smaller.

From Eq. 3 and 4, the half-angle of the Bragg envelope θ_(B) is definedas: $\begin{matrix}{\theta_{B} = \frac{\eta\lambda}{\pi\quad D\quad{\sin\left( \theta_{i} \right)}}} & {{Eq}.\quad 5}\end{matrix}$where η is a reflection efficiency factor which is the value for x inthe sinc²(x) function where the value of sinc²(x) has decreased to apredetermined value from the maximum amplitude as indicated by points204,206 on the curve 200.

We have found that the reflection efficiency is acceptable when η≦1.39.This value for η corresponds to when the amplitude of the reflected beam(i.e., from the sinc²(x) function of Eqs. 3 & 4) has decayed to about50% of its peak value. In particular, when x=1.39=η, sinc²(x)=0.5.However, other values for efficiency thresholds or factor in the Braggenvelope may be used if desired.

The beams 26-36 are imaged onto the CCD camera 60 to produce the patternof light and dark regions 120-132 representing a digital (or binary)code, where light=1 and dark=0 (or vice versa). The digital code may begenerated by selectively creating individual index variations (orindividual gratings) with the desired spatial periods Λ1-Λn. Otherillumination, readout techniques, types of gratings, geometries,materials, etc. may be used as discussed in the aforementioned patentapplication.

Referring to FIG. 12, illustrations (a)-(c), for the grating 12 in acylindrical substrate 10 having a sample spectral 17 bit code (i.e., 17different pitches Λ1-Λ17), the corresponding image on the CCD (ChargeCoupled Device) camera 60 is shown for a digital pattern of 7 bitsturned on (10110010001001001); 9 bits turned on of (11000101010100111);all 17 bits turned on of (11111111111111111).

For the images in FIG. 12, the length of the substrate 10 was 450microns, the outer diameter D1 was 65 microns, the inner diameter D was14 microns, δn for the grating 12 was about 10⁻⁴, n1 in portion 20 wasabout 1.458 (at a wavelength of about 1550 nm), n2 in portion 18 wasabout 1.453, the average pitch spacing Λ for the grating 12 was about0.542 microns, and the spacing between pitches ΔΛ was about 0.36% of theadjacent pitches Λ.

Referring to FIG. 13, illustration (a), the pitch Λ of an individualgrating is the axial spatial period of the sinusoidal variation in therefractive index n1 in the region 20 of the substrate 10 along the axiallength of the grating 12 as indicated by a curve 90 on a graph 91.Referring to FIG. 13, illustration (b), a sample composite grating 12comprises three individual gratings that are co-located on the substrate10, each individual grating having slightly different pitches, Λ1, Λ2,Λ3, respectively, and the difference (or spacing) ΔΛ between each pitchΛ being about 3.0% of the period of an adjacent pitch Λ as indicated bya series of curves 92 on a graph 94. Referring to FIG. 13, illustration(c), three individual gratings, each having slightly different pitches,Λ1, Λ2, Λ3, respectively, are shown, the difference ΔΛ between eachpitch Λ being about 0.3% of the pitch Λ of the adjacent pitch as shownby a series of curves 95 on a graph 97. The individual gratings in FIG.13, illustrations (b) and (c) are shown to all start at 0 forillustration purposes; however, it should be understood that, theseparate gratings need not all start in phase with each other. Referringto FIG. 13, illustration (d), the overlapping of the individualsinusoidal refractive index variation pitches Λ1-Λn in the gratingregion 20 of the substrate 10, produces a combined resultant refractiveindex variation in the composite grating 12 shown as a curve 96 on agraph 98 representing the combination of the three pitches shown in FIG.13, illustration (b). Accordingly, the resultant refractive indexvariation in the grating region 20 of the substrate 10 may not besinusoidal and is a combination of the individual pitches Λ (or indexvariation).

The maximum number of resolvable bits N, which is equal to the number ofdifferent grating pitches Λ (and hence the number of codes), that can beaccurately read (or resolved) using side-illumination and side-readingof the grating 12 in the substrate 10, is determined by numerousfactors, including: the beam width w incident on the substrate (and thecorresponding substrate length L and grating length Lg), the thicknessor diameter D of the grating 12, the wavelength λ of incident light, thebeam divergence angle θ_(R), and the width of the Bragg envelope θ_(B)(discussed more in the aforementioned patent application), and may bedetermined by the equation: $\begin{matrix}{N \cong \frac{{\eta\beta}\quad L}{2D\quad{\sin\left( \theta_{i} \right)}}} & {{Eq}.\quad 6}\end{matrix}$

Referring to FIG. 14, instead of having the input light 24 at a singlewavelength λ (monochromatic) and reading the bits by the angle θo of theoutput light, the bits (or grating pitches Λ) may be read/detected byproviding a plurality of wavelengths and reading the wavelength spectrumof the reflected output light signal. In this case, there would be onebit per wavelength, and thus, the code is contained in the wavelengthinformation of the reflected output signal.

In this case, each bit (or Λ) is defined by whether its correspondingwavelength falls within the Bragg envelope, not by its angular positionwithin the Bragg envelope 200. As a result, it is not limited by thenumber of angles that can fit in the Bragg envelope 200 for a givencomposite grating 12, as in the embodiment discussed hereinbefore. Thus,using multiple wavelengths, the only limitation in the number of bits Nis the maximum number of grating pitches Λ that can be superimposed andoptically distinguished in wavelength space for the output beam.

Referring to FIGS. 14 and 15, illustration (a), the reflectionwavelength spectrum (λ1-λn) of the reflected output beam 310 willexhibit a series of reflection peaks 695, each appearing at the sameoutput Bragg angle θo. Each wavelength peak 695 (λ1-λn) corresponds toan associated spatial period (Λ1-Λn), which make up the grating 12.

One way to measure the bits in wavelength space is to have the inputlight angle θi equal to the output light angle θo, which is kept at aconstant value, and to provide an input wavelength λ that satisfies thediffraction condition (Eq. 1) for each grating pitch Λ. This willmaximize the optical power of the output signal for each pitch Λdetected in the grating 12.

Referring to 15, illustration (b), the transmission wavelength spectrumof the transmitted output beam 330 (which is transmitted straightthrough the grating 12) will exhibit a series of notches (or dark spots)696. Alternatively, instead of detecting the reflected output light 310,the transmitted light 330 may be detected at the detector/reader 308. Itshould be understood that the optical signal levels for the reflectionpeaks 695 and transmission notches 696 will depend on the “strength” ofthe grating 12, i.e., the magnitude of the index variation n in thegrating 12.

In FIG. 14, the bits may be detected by continuously scanning the inputwavelength. A known optical source 300 provides the input light signal24 of a coherent scanned wavelength input light shown as a graph 304.The source 300 provides a sync signal on a line 306 to a known reader308. The sync signal may be a timed pulse or a voltage ramped signal,which is indicative of the wavelength being provided as the input light24 to the substrate 10 at any given time. The reader 308 may be aphotodiode, CCD camera, or other optical detection device that detectswhen an optical signal is present and provides an output signal on aline 309 indicative of the code in the substrate 10 or of thewavelengths present in the output light, which is directly related tothe code, as discussed herein. The grating 12 reflects the input light24 and provides an output light signal 310 to the reader 308. Thewavelength of the input signal is set such that the reflected outputlight 310 will be substantially in the center 314 of the Bragg envelope200 for the individual grating pitch (or bit) being read.

Alternatively, the source 300 may provide a continuous broadbandwavelength input signal such as that shown as a graph 316. In that case,the reflected output beam 310 signal is provided to a narrow bandscanning filter 318 which scans across the desired range of wavelengthsand provides a filtered output optical signal 320 to the reader 308. Thefilter 318 provides a sync signal on a line 322 to the reader, which isindicative of which wavelengths are being provided on the output signal320 to the reader and may be similar to the sync signal discussedhereinbefore on the line 306 from the source 300. In this case, thesource 300 does not need to provide a sync signal because the inputoptical signal 24 is continuous. Alternatively, instead of having thescanning filter being located in the path of the output beam 310, thescanning filter may be located in the path of the input beam 24 asindicated by the dashed box 324, which provides the sync signal on aline 323.

Alternatively, instead of the scanning filters 318,324, the reader 308may be a known optical spectrometer (such as a known spectrum analyzer),capable of measuring the wavelength of the output light.

The desired values for the input wavelengths λ (or wavelength range) forthe input signal 24 from the source 300 may be determined from the Braggcondition of Eq. 1, for a given grating spacing Λ and equal angles forthe input light θi and the angle light θo. Solving Eq. 1 for λ andplugging in m=1, gives:λ=Λ[sin(θo)+sin(θi)]  Eq. 7

It is also possible to combine the angular-based code detection with thewavelength-based code detection, both discussed hereinbefore. In thiscase, each readout wavelength is associated with a predetermined numberof bits within the Bragg envelope. Bits (or grating pitches Λ) writtenfor different wavelengths do not show up unless the correct wavelengthis used.

Accordingly, the bits (or grating pitches Λ) can be read using onewavelength and many angles, many wavelengths and one angle, or manywavelengths and many angles.

Referring to FIG. 16, the grating 12 may have a thickness or depth Dwhich is comparable or smaller than the incident beam wavelength λ. Thisis known as a “thin” diffraction grating (or the full angle Braggenvelope is 180 degrees). In that case, the half-angle Bragg envelope θBis substantially 90 degrees; however, π must be made large enough toprovide sufficient reflection efficiency, per Eqs. 3 and 4. Inparticular, for a “thin” grating, D*δn≈λ/2, which corresponds to a πphase shift between adjacent minimum and maximum refractive index valuesof the grating 12.

It should be understood that there is still a trade-off discussedhereinbefore with beam divergence angle θ_(R) and the incident beamwidth (or length L of the substrate), but the accessible angular spaceis theoretically now 90 degrees. Also, for maximum efficiency, the phaseshift between adjacent minimum and maximum refractive index values ofthe grating 12 should approach a π phase shift; however, other phaseshifts may be used.

In this case, rather than having the input light 24 coming in at theconventional Bragg input angle θi, as discussed hereinbefore andindicated by a dashed line 701, the grating 12 is illuminated with theinput light 24 oriented on a line 705 orthogonal to the longitudinalgrating vector 705. The input beam 24 will split into two (or more)beams of equal amplitude, where the exit angle θ_(o) can be determinedfrom Eq. 1 with the input angle θ_(i)0=0 (normal to the longitudinalaxis of the grating 12).

In particular, from Eq. 1, for a given grating pitch Λ1, the +/−1^(st)order beams (m=+1 and m=−1), corresponds to output beams 700,702,respectively. For the +/−2^(nd) order beams (m=+2 and m=−2), correspondsto output beams 704,706, respectively. The 0^(th) order (undefracted)beam (m=0), corresponds to beam 708 and passes straight through thesubstrate. The output beams 700-708 project spectral spots or peaks710-718, respectively, along a common plane, shown from the side by aline 709, which is parallel to the upper surface of the substrate 10.

For example, for a grating pitch Λ=1.0 um, and an input wavelength λ=400nm, the exit angles θ_(o) are ˜+/−23.6 degrees (for m=+/−1), and +/−53.1degrees (from m=+/−2), from Eq. 1. It should be understood that forcertain wavelengths, certain orders (e.g., m=+/−2) may be reflected backtoward the input side or otherwise not detectable at the output side ofthe grating 12.

Alternatively, one can use only the +/−1^(st) order (m=+/−1) outputbeams for the code, in which case there would be only 2 peaks to detect,712, 714. Alternatively, one can also use any one or more pairs from anyorder output beam that is capable of being detected. Alternatively,instead of using a pair of output peaks for a given order, an individualpeak may be used.

Referring to FIG. 17, if two pitches Λ1,Λ2 exist in the grating 12, twosets of peaks will exist. In particular, for a second grating pitch Λ2,the +/−st order beams (m=+1 and m=−1), corresponds to output beams720,722, respectively. For the +/−2^(nd) order beams (m=+2 and m=−2),corresponds to output beams 724,726, respectively. The 0^(th) order(un-defracted) beam (m=0), corresponds to beam 718 and passes straightthrough the substrate. The output beams 720-726 corresponding to thesecond pitch Λ2 project spectral spots or peaks 730-736, respectively,which are at a different location than the point 710-716, but along thesame common plane, shown from the side by the line 709.

Thus, for a given pitch Λ (or bit) in a grating, a set of spectral peakswill appear at a specific location in space. Thus, each different pitchcorresponds to a different elevation or output angle which correspondsto a predetermined set of spectral peaks. Accordingly, the presence orabsence of a particular peak or set of spectral peaks defines the code.

In general, if the angle of the grating 12 is not properly aligned withrespect to the mechanical longitudinal axis of the substrate 10, thereadout angles may no longer be symmetric, leading to possibledifficulties in readout. With a thin grating, the angular sensitivity tothe alignment of the longitudinal axis of the substrate 10 to the inputangle θi of incident radiation is reduced or eliminated. In particular,the input light can be oriented along substantially any angle θi withrespect to the grating 12 without causing output signal degradation, duethe large Bragg angle envelope. Also, if the incident beam 24 is normalto the substrate 10, the grating 12 can be oriented at any rotational(or azimuthal) angle without causing output signal degradation. However,in each of these cases, changing the incident angle θi will affect theoutput angle θo of the reflected light in a predetermined predictableway, thereby allowing for accurate output code signal detection orcompensation.

Referring to FIG. 18, for a thin grating, in addition to multiplexing inthe elevation or output angle based on grating pitch A, the bits canalso be multiplexed in an azimuthal (or rotational) angle ηa of thesubstrate. In particular, a plurality of gratings 750,752,754,756 eachhaving the same pitch Λ are disposed in a surface 701 of the substrate10 and located in the plane of the substrate surface 701. The inputlight 24 is incident on all the gratings 750,752,754,756 simultaneously.Each of the gratings provides output beams oriented based on the gratingorientation. For example, the grating 750 provides the output beams764,762, the grating 752 provides the output beams 766,768, the grating754 provides the output beams 770,772, and the grating 756 provides theoutput beams 774,776. Each of the output beams provides spectral peaksor spots (similar to that discussed hereinbefore), which are located ina plane 760 that is parallel to the substrate surface plane 701. In thiscase, a single grating pitch Λ can produce many bits depending on thenumber of gratings that can be placed at different azimuthal(rotational) angles on the surface of the substrate 10 and the number ofoutput beam spectral peaks that can be spatially and opticallyresolved/detected. Each bit may be viewed as the presence or absence ofa pair of peaks located at a predetermined location in space in theplane 760. Note that this example uses only the m=+/−1^(st) order foreach reflected output beam. Alternatively, the detection may also usethe m=+/−2nd order. In that case, there would be two additional outputbeams and peaks (not shown) for each grating (as discussed hereinbefore)that may lie in the same plane as the plane 760 and may be on aconcentric circle outside the circle 760.

In addition, the azimuthal multiplexing can be combined with theelevation or output angle multiplexing discussed hereinbefore to providetwo levels of multiplexing. Accordingly, for a thin grating, the numberof bits can be multiplexed based on the number of grating pitches Λand/or geometrically by the orientation of the grating pitches.

Furthermore, if the input light angle θi is normal to the substrate 10,the edges of the substrate 10 no longer scatter light from the incidentangle into the “code angular space”, as discussed herein and/or in theaforementioned patent application.

Also, in the thin grating geometry, a continuous broadband wavelengthsource may be used as the optical source if desired.

Referring to FIG. 19, instead of or in addition to the pitches Λ in thegrating 12 being oriented normal to the longitudinal axis, the pitchesmay be created at a angle θg. In that case, when the input light 24 isincident normal to the surface 792, will produce a reflected output beam790 having an angle θo determined by Eq. 1 as adjusted for the blazeangle θg. This can provide another level of multiplexing bits in thecode.

Referring to FIG. 20, instead of using an optical binary (0-1) code, anadditional level of multiplexing may be provided by having the opticalcode use other numerical bases, if intensity levels of each bit are usedto indicate code information. This could be achieved by having acorresponding magnitude (or strength) of the refractive index change(δn) for each grating pitch A. Four intensity ranges are shown for eachbit number or pitch A, providing for a Base-4 code (where each bitcorresponds to 0, 1, 2, or 3). The lowest intensity level, correspondingto a 0, would exist when this pitch Λ is not present in the grating 12.The next intensity level 450 would occur when a first low level δn2exists in the grating that provides an output signal within theintensity range corresponding to a 1. The next intensity level 452 wouldoccur when a second higher level δn2 exists in the grating 12 thatprovides an output signal within the intensity range corresponding to a2. The next intensity level 452, would occur when a third higher levelδn3 exists in the grating 12 that provides an output signal within theintensity range corresponding to a 3.

Referring to FIG. 21, the input light 24 may be incident on thesubstrate 10 on an end face 600 of the substrate 10. In that case, theinput light 24 will be incident on the grating 12 having a moresignificant component of the light (as compared to side illuminationdiscussed hereinbefore) along the longitudinal grating axis 207 of thegrating (along the grating vector k_(B)), as shown by a line 602. Thelight 602 reflects off the grating 12 as indicated by a line 604 andexits the substrate as output light 608. Accordingly, it should beunderstood by one skilled in the art that the diffraction equationsdiscussed hereinbefore regarding output diffraction angle θo also applyin this case except that the reference axis would now be the gratingaxis 207. Thus, in this case, the input and output light angles θi,θo,would be measured from the grating axis 207 and length Lg of the grating12 would become the thickness or depth D of the grating 12. As a result,a grating 12 that is 400 microns long, would result in the Braggenvelope 200 being narrow. It should be understood that because thevalues of n1 and n2 are close to the same value, the slight anglechanges of the light between the regions 18,20 are not shown herein.

In the case where incident light 610 is incident along the samedirection as the grating vector (Kb) 207, i.e., θi=0 degrees, theincident light sees the whole length Lg of the grating 12 and thegrating provides a reflected output light angle θo=0 degrees, and theBragg envelope 612 becomes extremely narrow, as the narrowing effectdiscussed above reaches a limit. In that case, the relationship betweena given pitch Λ in the grating 12 and the wavelength of reflection λ isgoverned by a known “Bragg grating” relation:λ=2n _(eff)Λ  Eq. 8where n_(eff) is the effective index of refraction of the substrate, λis the input (and output wavelength) in free space (or vacuum) and Λ isthe pitch. This relation, as is known, may be derived from Eq. 1 whereθi=θo=90 degrees.

In that case, the code information is readable only in the spectralwavelength of the reflected beam, similar to that discussed hereinbeforefor wavelength based code reading. Accordingly, the input signal in thiscase may be a scanned wavelength source or a broadband wavelengthsource. In addition, as discussed hereinbefore for wavelength based codereading, the code information may be obtained in reflection from thereflected beam 614 or in transmission by the transmitted beam 616 thatpasses through the grating 12.

It should be understood that for shapes of the substrate 10 or element 8other than a cylinder, the effect of various different shapes on thepropagation of input light through the element 8, substrate 10, and/orgrating 12, and the associated reflection angles, can be determinedusing known optical physics including Snell's Law, shown below:n_(in) sin θin=n_(out) sin θout  Eq. 9

-   -   where n_(in) is the refractive index of the first (input)        medium, and n_(out) is the refractive index of the second        (output) medium, and θin and θout are measured from a line 620        normal to an incident surface 622.

Referring to FIG. 22, if the value of n1 in the grating region 20 isgreater than the value of n2 in the non-grating region 18, the gratingregion 20 of the substrate 10 will act as a known optical waveguide forcertain wavelengths. In that case, the grating region 20 acts as a“core” along which light is guided and the outer region 18 acts as a“cladding” which helps confine or guide the light. Also, such awaveguide will have a known “numerical aperture” (θna) that will allowlight that is within the aperture θna to be directed or guided along thegrating axis 207 and reflected axially off the grating 12 and returnedand guided along the waveguide. In that case, the grating 12 willreflect light having the appropriate wavelengths related to the pitchesΛ present in the grating 12 (as defined in Eq. 8) back along the region20 (or core) of the waveguide, and will pass the remaining wavelengthsof light as the light 632. Thus, having the grating region 20 act as anoptical waveguide for wavelengths reflected by the grating 12 allowsincident light that is not aligned exactly with the grating axis 207 tobe guided along and aligned with the grating 12 axis 207 for optimalgrating reflection.

If an optical waveguide is used any standard waveguide may be used,e.g., a standard telecommunication single mode optical fiber (125 microndiameter or 80 micron diameter fiber with about a 8-10 micron diameter),or a larger diameter waveguide (greater than 0.5 mm diameter), such asis describe in U.S. patent application Ser. No. 09/455,868, filed Dec.6, 1999, entitled “Large Diameter Waveguide, Grating”. Further, any typeof optical waveguide may be used for the optical substrate 10, such as,a multi-mode, birefringent, polarization maintaining, polarizing,multi-core, multi-cladding, or microsturctured optical waveguide, or aflat or planar waveguide (where the waveguide is rectangular shaped), orother waveguides.

Referring to FIG. 23, if the grating 12 extends across the entiredimension D of the substrate, the substrate 10 does not behave as awaveguide for the incident or reflected light and the incident light 24will be diffracted (or reflected) as indicated by lines 642, and thecodes detected as discussed hereinbefore for the end-incidence conditiondiscussed hereinbefore with FIG. 45, and the remaining light 640 passesstraight through.

Referring to FIG. 24, illustrations (a)-(c), in illustration (a), forthe end illumination condition, if a blazed or angled grating is used,as discussed hereinbefore, the input light 24 is coupled out of thesubstrate 10 at a known angle as shown by a line 650. Referring to FIG.24, illustration (b), alternatively, the input light 24 may be incidentfrom the side and, if the grating 12 has the appropriate blaze angle,the reflected light will exit from the end face 652 as indicated by aline 654. Referring to FIG. 24, illustration (c), the grating 12 mayhave a plurality of different pitch angles 660,662, which reflect theinput light 24 to different output angles as indicated by lines 664,666. This provides another level of multiplexing (spatially) additionalcodes, if desired.

The grating 12 may be impressed in the substrate 10 by any technique forwriting, impressed, embedded, imprinted, or otherwise forming adiffraction grating in the volume of or on a surface of a substrate 10.Examples of some known techniques are described in U.S. Pat. Nos.4,725,110 and 4,807,950, entitled “Method for Impressing Gratings WithinFiber Optics”, to Glenn et al; and U.S. Pat. No. 5,388,173, entitled“Method and Apparatus for Forming Aperiodic Gratings in Optical Fibers”,to Glenn, respectively, and U.S. Pat. No. 5,367,588, entitled “Method ofFabricating Bragg Gratings Using a Silica Glass Phase Grating Mask andMask Used by Same”, to Hill, and U.S. Pat. No. 3,916,182, entitled“Periodic Dielectric Waveguide Filter”, Dabby et al, and U.S. Pat. No.3,891,302, entitled “Method of Filtering Modes in Optical Waveguides”,to Dabby et al, which are all incorporated herein by reference to theextent necessary to understand the present invention.

Alternatively, instead of the grating 12 being impressed within thesubstrate material, the grating 12 may be partially or totally createdby etching or otherwise altering the outer surface geometry of thesubstrate to create a corrugated or varying surface geometry of thesubstrate, such as is described in U.S. Pat. No. 3,891,302, entitled“Method of Filtering Modes in Optical Waveguides”, to Dabby et al, whichis incorporated herein by reference to the extent necessary tounderstand the present invention, provided the resultant opticalrefractive profile for the desired code is created.

Further, alternatively, the grating 12 may be made by depositingdielectric layers onto the substrate, similar to the way a known thinfilm filter is created, so as to create the desired resultant opticalrefractive profile for the desired code.

The substrate 10 (and/or the element 8) may have end-viewcross-sectional shapes other than circular, such as square, rectangular,elliptical, clam-shell, D-shaped, or other shapes, and may haveside-view sectional shapes other than rectangular, such as circular,square, elliptical, clam-shell, D-shaped, or other shapes. Also, 3Dgeometries other than a cylinder may be used, such as a sphere, a cube,a pyramid or any other 3D shape. Alternatively, the substrate 10 mayhave a geometry that is a combination of one or more of the foregoingshapes.

The shape of the element 8 and the size of the incident beam may be madeto minimize any end scatter off the end face(s) of the element 8, as isdiscussed herein and/or in the aforementioned patent application.Accordingly, to minimize such scatter, the incident beam 24 may be ovalshaped where the narrow portion of the oval is smaller than the diameterD1, and the long portion of the oval is smaller than the length L of theelement 8. Alternatively, the shape of the end faces may be rounded orother shapes or may be coated with an antireflective coating.

It should be understood that the size of any given dimension for theregion 20 of the grating 12 may be less than any corresponding dimensionof the substrate 10. For example, if the grating 12 has dimensions oflength Lg, depth Dg, and width Wg, and the substrate 12 has differentdimensions of length L, depth D, and width W, the dimensions of thegrating 12 may be less than that of the substrate 12. Thus, the grating12, may be embedded within or part of a much larger substrate 12. Also,the element 8 may be embedded or formed in or on a larger object foridentification of the object.

The dimensions, geometries, materials, and material properties of thesubstrate 10 are selected such that the desired optical and materialproperties are met for a given application. The resolution and range forthe optical codes are scalable by controlling these parameters asdiscussed herein and/or in the aforementioned patent application.

Referring to FIG. 25, the substrate 10 may have an outer coating 799,such as a polymer or other material that may be dissimilar to thematerial of the substrate 10, provided that the coating 799 on at leasta portion of the substrate, allows sufficient light to pass through thesubstrate for adequate optical detection of the code. The coating 799may be on any one or more sides of the substrate 10. Also, the coating799 may be a material that causes the element 8 to float or sink incertain fluids (liquid and/or gas) solutions.

Also, the substrate 10 may be made of a material that is less dense thancertain fluid (liquids and/or gas) solutions, thereby allowing theelements 8 to float or be buoyant or partially buoyant. Also, thesubstrate may be made of a porous material, such as controlled poreglass (CPG) or other porous material, which may also reduce the densityof the element 8 and may make the element 8 buoyant or partially-buoyantin certain fluids.

Referring to FIG. 26, the grating 12 is axially spatially invariant. Asa result, the substrate 10 with the grating 12 (shown as a longsubstrate 21) may be axially subdivided or cut into many separatesmaller substrates 30-36 and each substrate 30-36 will contain the samecode as the longer substrate 21 had before it was cut. The limit on thesize of the smaller substrates 30-36 is based on design and performancefactors discussed herein and/or in the aforementioned patentapplication.

Referring to FIG. 27, one purpose of the outer region 18 (or regionwithout the grating 12) of the substrate 10 is to provide mechanical orstructural support for the inner grating region 20. Accordingly, theentire substrate 10 may comprise the grating 12, if desired.Alternatively, the support portion may be completely or partiallybeneath, above, or along one or more sides of the grating region 20,such as in a planar geometry, or a D-shaped geometry, or othergeometries, as described herein and/or in the aforementioned patentapplication. The non-grating portion 18 of the substrate 10 may be usedfor other purposes as well, such as optical lensing effects or othereffects (discussed herein or in the aforementioned patent application).Also, the end faces of the substrate 10 need not be perpendicular to thesides or parallel to each other. However, for applications where theelements 8 are stacked end-to-end, the packing density may be optimizedif the end faces are perpendicular to the sides.

Referring to FIGS. 28, illustrations (a)-(c), two or more substrates10,250, each having at least one grating therein, may be attachedtogether to form the element 8, e.g., by an adhesive, fusing or otherattachment techniques. In that case, the gratings 12,252 may have thesame or different codes.

Referring to FIGS. 29, illustrations (a) and (b), the substrate 10 mayhave multiple regions 80,90 and one or more of these regions may havegratings in them. For example, there may be gratings 12,252 side-by-side(illustration (a)), or there may be gratings 82-88, spaced end-to-end(illustration (b)) in the substrate 10.

Referring to FIG. 30, the length L of the element 8 may be shorter thanits diameter D, thus, having a geometry such as a plug, puck, wafer,disc or plate.

Referring to FIG. 31, to facilitate proper alignment of the grating axiswith the angle θi of the input beam 24, the substrate 10 may have aplurality of the gratings 12 having the same codes written therein atnumerous different angular or rotational (or azimuthal) positions of thesubstrate 10. In particular, two gratings 550, 552, having axial gratingaxes 551, 553, respectively may have a common central (or pivot orrotational) point where the two axes 551,553 intersect. The angle θi ofthe incident light 24 is aligned properly with the grating 550 and isnot aligned with the grating 552, such that output light 555 isreflected off the grating 550 and light 557 passes through the grating550 as discussed herein. If the element 8 is rotated as shown by thearrows 559, the angle θi of incident light 24 will become alignedproperly with the grating 552 and not aligned with the grating 550 suchthat output light 555 is reflected off the grating 552 and light 557passes through the grating 552. When multiple gratings are located inthis rotational orientation, the bead may be rotated as indicated by aline 559 and there may be many angular positions that will providecorrect (or optimal) incident input angles θi to the grating. While thisexample shows a circular cross-section, this technique may be used withany shape cross-section.

Referring to FIG. 32, illustrations (a), (b), (c), (d), and (e) thesubstrate 10 may have one or more holes located within the substrate 10.In illustration (a), holes 560 may be located at various points alongall or a portion of the length of the substrate 10. The holes need notpass all the way through the substrate 10. Any number, size and spacingfor the holes 560 may be used if desired. In illustration (b), holes 572may be located very close together to form a honeycomb-like area of allor a portion of the cross-section. In illustration (c), one (or more)inner hole 566 may be located in the center of the substrate 10 oranywhere inside of where the grating region(s) 20 are located. The innerhole 566 may be coated with a reflective coating 573 to reflect light tofacilitate reading of one or more of the gratings 12 and/or to reflectlight diffracted off one or more of the gratings 12. The incident light24 may reflect off the grating 12 in the region 20 and then reflect offthe surface 573 to provide output light 577. Alternatively, the incidentlight 24 may reflect off the surface 573, then reflect off the grating12 and provide the output light 575. In that case the grating region 20may run axially or circumferentially 571 around the substrate 10. Inillustration (d), the holes 579 may be located circumferentially aroundthe grating region 20 or transversely across the substrate 10. Inillustration (e), the grating 12 may be located circumferentially aroundthe outside of the substrate 10, and there may be holes 574 inside thesubstrate 10.

Referring to FIG. 33, illustrations (a), (b), and (c), the substrate 10may have one or more protruding portions or teeth 570, 578,580 extendingradially and/or circumferentially from the substrate 10. Alternatively,the teeth 570, 578,580 may have any other desired shape.

Referring to FIG. 34, illustrations (a), (b), (c) a D-shaped substrate,a flat-sided substrate and an eye-shaped (or clam-shell or teardropshaped) substrate 10, respectively, are shown. Also, the grating region20 may have end cross-sectional shapes other than circular and may haveside cross-sectional shapes other than rectangular, such as any of thegeometries described herein for the substrate 10. For example, thegrating region 20 may have a oval cross-sectional shape as shown bydashed lines 581, which may be oriented in a desired direction,consistent with the teachings herein. Any other geometries anddimensions for the substrate 10 or the grating region 20 may be used ifdesired, as described herein. For example, other dimensions that we havefound useful are D1=about 25-30 microns, and D=about 6-8 microns andlength L=about 230-260 microns. Any other dimensions may be used ifdesired, provided it meets the performance requirements of theapplication.

Referring to FIG. 35, at least a portion of a side of the substrate 10may be coated with a reflective coating to allow incident light 510 tobe reflected back to the same side from which the incident light came,as indicated by reflected light 512.

Referring to FIG. 36, illustrations (a) and (b), alternatively, thesubstrate 10 can be electrically and/or magnetically polarized, by adopant or coating, which may be used to ease handling and/or alignmentor orientation of the substrate 10 and/or the grating 12, or used forother purposes. Alternatively, the bead may be coated with conductivematerial, e.g., metal coating on the inside of a holy substrate, ormetallic dopant inside the substrate. In these cases, such materials cancause the substrate 10 to align in an electric or magnetic field.Alternatively, the substrate can be doped with an element or compoundthat fluoresces or glows under appropriate illumination, e.g., a rareearth dopant, such as Erbium, or other rare earth dopant or fluorescentor luminescent molecule. In that case, such fluorescence or luminescencemay aid in locating and/or aligning substrates.

Referring to FIGS. 37-40, in addition, the elements 8 may be used tolabel drugs, or other medical, pharmaceutical, health care or cosmeticsproducts, and/or the packages or containers they are supplied with (asused herein, the term “drug” shall include such products). Such labelingcan provide product identification at the pill (or liquid) level orpackage/container level, which provides traceability of these productsto their manufacturer, thereby reducing counterfeit products in themarketplace.

Referring to FIG. 37, 38, one or more beads 8 can be located insideand/or on the outer surface of a pill or capsule 900, e.g., asolid/powder pill or a liquid/gel/fluid pill. The beads 8 may beinserted into the manufacturing process for the pill 900 at a convenientpoint in the process, such as when the pill 900 is in a wet or drygranular stage in the process.

Referring to FIGS. 39, 40, alternatively, the grating 12 itself may beembedded or written directly into the outer surface or coating of thepills 900, e.g., by photo-imprinting the grating 12 directly into thesurface coating material. In that case, there may be in a membrane orcoating surrounding part or all of the pill, or in the case of acapsule-type pill, the diffraction grating 12 may be disposed directlyin the casing of the capsule. Also, the coating or casing would have thenecessary material properties, such as photosensitivity, to allow thegrating 12 to be imprinted therein. Material properties are described incopending US patent application, publication number: WO 2004/025559;PCT/US 03/28874 (CV-0038A) and WO 2004/025344 A1; PCT/US 03/28890(CV-0044) and techniques for photo-imprinting are described in US patentapplication, publication number; WO 2004/025344 A1; PCT/US 03/028890(CV-0044) which is incorporated herein by reference in its entirety.

Referring to FIG. 41, alternatively, the beads 8 may be disposed withina liquid medicine 902 contained in a container 904.

Referring to FIGS. 42, 43, alternatively, one or more of the beads 8 maybe placed within the material of a container/package 903, 904 for thepills 900, such as a blister pack 903 (FIG. 42), a pill bottle 905 (FIG.43), or a liquid medicine container 904 (FIG. 41), or other pillcontainer/package. In that case, the beads 8 may be disposed on or inthe container/package material or the grating 12 itself may be embeddeddirectly into the container/package material, e.g., by photo-imprintingthe grating 12 directly into the container/package material.

For any of the embodiments herein, if the beads 8 or gratings 12 aredisposed against or near a surface that is reflective to the incidentlight, the codes in the beads 8 or gratings 12 may be read inreflection. For example, in the case of the blister pack 903, areflective under surface (or coating or backing) 906 may be used.Aluminum foil is commonly used as a backing for blister packs to holdthe pills 900 in the blistered/bubbled sections 905 of the package 903,which may be used as a reflective surface. In that case, the beads 8 orgrating 12 may be placed within the clear plastic material above thereflective backing, thereby allowing the beads 8 or grating 12 to beread in reflection from the upper surface.

Alternatively, the beads 8 may be coated with a material that reducesinteraction with the body, or that allows a human or animal to ingestthe beads 8 and pass them through urine or stool or allows the beads 8to be injected into the body or blood stream and monitored.Alternatively, the beads 8 may be of a material that is chewable ordissolves in the body or made of a material that will not harm the body.

In the case where beads 8 are embedded in the item, the beads can beidentified by destroying the item or a portion thereof to obtain thebeads 8. For example, in the case of a pill 900, the pill 900 may beplaced in a solution that dissolves the pill 900 but does not dissolvethe beads 8. For example, for glass beads 8, hot sulfuric acid or otheracid may be used to dissolve the pill 900 but will not harm the beads 8.For beads 8 made of other materials, such as polymers, hot water orother solutions may be used to dissolve the pill 900. Once the pill 900has been dissolved, the liquid containing the dissolved pill 900 and thebeads 8 may be pipetted into a bead reader to read the bead codes, suchas that described in US patent applications, publication numbers: WO2004/025559; PCT/US 03/28874 (CV-0038A), WO 2004/024328; PCT/US 03/28862(CV-0042), WO 2004/066210; PCT/US 04/01685 (CV-0054), and WO2005/033681; PCT/US 04/032084 (CV-0092), which are all incorporatedherein by reference in their entirety. However, any type of readercapable of reading the beads 8 may be used. Alternatively, the liquidmay be poured through a filter or screen to isolate the beads 8 then putinto a bead reader to read the bead codes.

Referring to FIG. 44-54 and 44A and 51A, the elements 8 may be embeddedinto a film (or coating, wrapping, sheet, tape, or the like) 910. Inthat case, the film 910 would be made of any material that issubstantially transparent to the wavelength of incident light used toread the code in the element 8, sufficient to allow the optical codesignal to be detected. Some examples are polymers or plastics, but anyother material may be used that meets the functional requirementsdescribed herein. In that case, the elements 8 would lay substantiallyflat. The liquid film material may be applied (e.g., by spreading,spraying, extruding, or any other application technique) onto a surfaceand the elements 8 applied into the liquid and/or the elements 8 may bepre-mixed into the liquid prior to being applied to the surface. Thesurface may be a final surface to be coated or an intermediate surfacefrom which the film is removed and stored or rolled for later use.

Referring to FIG. 44, the elements 8 may have a random orientation inthe film 910. Referring to FIGS. 44A, 45, 46, alternatively, theelements 8 may be aligned in the film 910 along one or more axes alongstraight lines or curved lines or grid-like, or have any 1-dimensionalor 2-dimensional random or non-random pattern or shape, such as thosepatterns shown in FIG. 45.

Alignment of the elements 8 may be achieved using vibration, pressurewaves, acoustic waves, air movement, electric or magnetic fields, and/orcentripetal force, when the film 910 is in liquid form prior to curing.In particular, the underlying surface may be disposed on a vibration orshaker table which oscillates back and forth thereby creating a standingwave in the liquid along which the elements 8 will align along apredetermined axis. One technique for bead alignment and or movement isdescribed in copending patent applications Serial Nos. (CyVera DocketNo. CV-0086 PR and CV-0087 PR) referenced herein and incorporated byreference.

Alternatively, a cover sheet or plate may be placed on the surface ofthe film and pressure waves created along the liquid film, similar tothat discussed in the co-pending patent applications Serial Nos. (CyVeraDocket No. CV-0086 PR and CV-0087 PR) referenced herein and incorporatedby reference. Alternatively, a pulsed or continuous air stream may beblown across the surface of the liquid, creating a standing wave in theliquid along which the elements 8 will align. Alternatively, forelements 8 having an electric and/or magnetic polarization, as discussedherein with FIG. 36 and/or in the aforementioned patent applications,the elements 8 may be aligned using an electric and/or magnetic fieldapplied across the liquid. Alternatively, centripetal force may be usedto align the elements 8 by spinning the surface in a predetermineddirection.

Referring to FIG. 46, the elements 8 may be aligned by using physicalmechanical alignment such as grooves (or corrugations or ripples orlines or walls) 912 in the surface of the underlying material 914. Inthat case, the elements 8 would be laid on the grooved surface wouldfall into and align along the grooves, and then the coating 916 would beapplied over the elements and grooves. Alternatively, the elements 8 maybe applied to the material after the coating 916 is applied and theelements 8 would settle into the grooves. The longitudinal axis of thegrooves 912 may run along straight lines or curved lines or grid-like,or have any 1-dimensional or 2-dimensional predetermined or randompattern or shape. Some non-limiting examples of groove patterns areshown in FIG. 45, any other patterns may be used if desired. Also, thesepatterns may be on separate sheets or on one sheet or overlapping orspatially separated. For two-dimensional patterns, the elements 8 maylay in the outline of the pattern or fill in all or any portion of thepattern.

Referring to FIG. 48, the length of the elements 8 are determined by theapplication. For example, the elements 8 may be particle size (e.g.,less than about 1000 microns in length and less than about 1000 micronsin diameter), or longer filaments or thread 918 having a length L longerthan about 1000 microns and a diameter or thickness D less than about250 microns.

Referring to FIG. 44A, alternatively, if the elements 8 are filaments918, the filaments 918 may be held in tension in parallel to createalignment and the coating 916 may be applied to the filaments and, afterthe coating 916 hardens, the tension may be removed and the filamentswill be aligned within the coating.

The patterns discussed herein may be partially or completely made fromencoded optical identification elements 8 having a particle size or alonger filament length or a combination of both. The maximum number ofbits for each code increases as the length of the filament increases asdiscussed herein and/or in the copending patent application, publicationnumber: WO 2004/025559; PCT/US 03/28874 (CV-0038A).

Referring to FIGS. 51, 51A, 52, 53, alternatively, the elements 8 may bepre-aligned on or within a substantially transparent adhesive film oradhesive tape 920, similar to standard transparent adhesive tape 920. Inthat case, the tape 920 may be rolled on itself as shown by a roll (orreel or spool) 922 and then a predetermined amount of tape removed fromthe roll and adhered to a desired item or package. The film 920 may bemade if any material that is substantially transparent to the wavelengthof incident light used to read the code in the element 8, sufficient toallow the optical code signal to be detected.

The underlying item or package to which the transparent film/tape 920 isapplied may be made of a material that is substantially transparent tothe wavelength of incident light used to read the code in the element 8,sufficient to allow the optical code signal to be detected. In thatcase, the code may be read in transmission, i.e., the incident light onone side of the element and code beam and detector on the other side.However, if the underlying surface material is not sufficientlytransparent to read the code in transmission, the code may be read inreflection. In that case, the surface of the underlying material wouldbe made of a material that reflects the diffracted incident lightsufficient to allow the code to be detected from the same side as theincident light (discussed more hereinafter).

Also, instead of or in addition to disposing the elements 8 in the film910, the film may have the diffraction grating 12 disposed directly inor on the film 910. In that case, the diffraction grating 12 would havean orientation and length/dimensions as desired.

Referring to FIG. 47, also, the elements 8 may be mixed with a liquidcarrier or resin 926 which may applied to an item 924 to be labeled. Theliquid carrier 926 with the elements 8 located therein may be appliedusing markers, pens, brushes, air brushes, liquid brushes, fluidbrushes, injection molding, extrusion or any other device or techniquethat allows the liquid and beads to be applied. The elements 8 may beused or applied in a spot or coverage area 928 having a predeterminedsize and geometry using a substantially transparent carrier materialthat is applied to the surface of the item 924.

Referring to FIG. 50, the elements 8 may also be used on labels toauthenticate a label, e.g., on a box, package, container, document,product, or the like. In that case, any of the techniques discussedherein may be used to apply the elements to the label. It may be used onany kind of label including bar code labels. The elements 8 may also beused on or within seals and shrink-wraps.

The elements 8 may be used in compound resins (such as acrylic,polypropylene, polycarbonate, polyethelene, polystyrene, and the like)as well as plastic resins. Also, the elements 8 can be incorporated intopulp during paper manufacturing processes.

Referring to FIGS. 49 and 50, a piece of the tape 920 can be applied tothe surface of the parcel or item 924,926 and used as a tag 922. Also,the tape 920 can be designed to make it very difficult to find if thelocation of the tag 922 if the location was not already known, e.g., fora transparent tag. Since both the tape and the encoded filaments withinthe tape may be transparent to the naked eye and could be made small (1mm×1 mm) it may be very difficult to locate the tag 922 by eye. Anyother size may be used if desired. Once located, the tag 922 wouldrequire a special reader to interrogate the code. The tag 922 could belaminated over with any transparent material to ensure that it could notbe easily removed once affixed.

Referring to FIGS. 52, the filaments 918 may be embedded perpendicularto the longitudinal axis of the tape 920 to produce a roll or spool 922of the tape 920 with a series of sections 930 having serialized codes,wherein a given section 930 of predetermined length Lt and width Wtwould contain a set of filaments all with the same code. Each of thesections 930 may contain a set of filaments each having a differentcode. Referring to FIG. 52, to fabricate a large number of such spools,the spool 922 of the tape 920 could be cut along the dashed lines 931into smaller width spools as shown in FIG. 53. Referring to FIG. 51, ifa single spool 922 with the same code is desired, the encoded filaments918 could be arranged parallel to the longitudinal axis of the tape 920.Referring to FIG. 51A, it is also possible to make the tape roll 920where the encoded filaments 918 are arranged in multiple orientations,such as parallel, perpendicular, and/or at 45 degrees or any otherangular orientations. In that case, the filaments 918 may be laid on topof each other in the various orientations (see FIG. 51A) or on separateareas or portions of the tape 920 or a combination of each.

The codes can be sectioned and segmented however desired. Also, within asection 930 of the tape 920, there may be redundant filaments with thesame code for authentication, validation and/or error checking purposes.

The above discussion regarding the tape 920 using elements 8 asfilaments may also be used with the elements 8 having a particle size ifdesired or a combination of each.

Referring to FIGS. 54-65, when a reflective surface (or layer, coating,backing, or the like) 906 is used under the diffraction grating, variousconfigurations may be used for reading the code. Referring to FIG. 54,in certain configurations, the reflective surface 906 may cause aninterference effect between a reflected code beam 935 and a second codebeam 932 shown as an overlap area 934. This interference distorts theprimary code beam 935 thereby causing a potential error in reading thecode.

In particular, the code beam 27 reflects off the reflective surface 906as a reflected beam 935 which is incident on the back side of thegrating 12. A portion of the reflected beam 935 passes straight throughthe grating 12 as the primary code beam 935. Also, a small portion (notshown) of the reflected beam 935 is diffracted by the grating 12. Thebeam 25 from the incident beam 24 that passes through the grating 12 isreflected off the reflective surface 906 as a reflected beam 933 whichis incident on the back side of the grating 12. A portion of thereflected beam 933 passes straight through the grating 12 as the beam937 and a small portion of the reflected beam 933 is diffracted by thegrating 12 as the second code beam 932. The interference is caused bythe intersection of the primary and secondary code beams 935, 932,respectively, cause the interference effect. However, there are severalapproaches that can minimize or eliminate this effect.

Referring to FIG. 55, one way to minimize or eliminate the interferenceeffect is to put in an aperture device 936 having a blocking section 938to block the second code beam 932 from interfering with the main codebeam 27 and an aperture (or hole) section 940 to allow the incident beam24 to pass. The aperture 936 may be placed near the element 8.Alternatively, the optical signal at the element 8 may be imaged toanother location where the aperture 936 may be placed.

Referring to FIG. 56, alternatively, the spacing or distance(Dseparation) between the diffraction grating 12 and the reflectivesurface 906 may be made such that the first and second code beams27,932, respectively, do not interfere. This may be done by making theouter portion 10 of the element 8 large enough or by placing the element8 far enough away from the reflective surface 906.

The amount and location of overlap (and thus interference) between theprimary and secondary beams 935 and 932 may be determined by thedistance Dreflector between the grating 12 and the reflective surface906. If Dreflector is large enough such that the total distance traveledby the passed beam 25 and the reflected beam 933 is greater than about 2Rayleigh ranges, then the reflected beam 933 has become diverged enoughsuch that the intensity of the second code beam is low enough not tocause significant interference with the primary beam. Thus, in thatcase, the aperture device 936 is not required. For this “divergent beam”condition to exist the following should be true:Dreflector>>1.3*BeamWidth/4(sin(θincident_medium))  Eq. 10

-   -   where BeamWidth is the 1/e² times the full width of the beam,        and θincident_medium is the angle of the incident beam within        the grating 12.

If the distance Dreflector is smaller than the condition set by Eq. 10,some level of interference may occur. In that case, the aperture device936 discussed hereinbefore may be used, provided the following conditionis met:Dbeam_separation≧1.3*BeamWidth/cos(θincident_medium))  Eq. 11where Dbeam_separataion is the distance between the center of theprimary and secondary code beams 932,935; and where:Dbeam_separation=4*Dreflector* Tan(θincident_medium)  Eq. 12Therefore, the aperture device 936 can be used when:Dreflector≧1.3*BeamWidth/4(Sin(θincident_medium))  Eq. 13

Referring to FIG. 57, a plot 942 of a normalized Gaussian beam having a1/e² full width of 2 is shown. The factor 1.3 in Eq. 13 is a clearancefactor based on the standard minimum aperture hole size used forGaussian beams in order to minimize aperture effects, such asattenuation, diffraction, beam shape, and the like, in the far field.This shows the decrease in beam power loss when going from a value of 1to a value of 1.3 for the clearance factor.

Referring to FIG. 66, alternatively, the grating 12 may be a blazedgrating to help avoid the interference between the primary and secondarycode beams. Also see FIG. 19 for a description of use of a blazedgrating. In particular, the incident beam 24 will diffract off theblazed grating 12 based on the blaze angle θ_(G) but the reflected beam933 does not diffract off the blazed grating as it is more aligned withthe blaze angle θ_(G) and thus much less diffraction will occur. As aresult, the second code beam 932 will have a much lower intensity,resulting in reduced or eliminated interference with the primary codebeam 935. It should be understood that in the case of a blazed gratingthe rotational (or azimuthal) orientation of the grating 12 should bepreserved, which may be achieved when the elements 8 are aligned andheld in place, such as with a resin or coating or tape as discussedherein.

Referring to FIGS. 58,59,60, alternatively, the reflective surface maybe tilted relative to a horizontal reference plane 931 to prevent thetwo code beams from interfering. FIG. 58 shows no tilt (zero degrees)and shows the two code beam angles as the same value of 32 degrees fromthe normal. Referring to FIG. 59, a 1 degree tilt produces an angle of30 degrees from the normal for the primary code beam and 30.04 degreesfor the secondary code beam. Referring to FIG. 60, a 5 degree tiltproduces an angle of 22 degrees from the normal for the primary codebeam and 23 degrees for the secondary code beam. The two code beams willnot interfere in the far field if their angles of incidence aresufficiently different and this angle difference is greater than thebeam divergence, even if they overlap in space in the near field. Forexample, in FIG. 59, a 0.04 degree difference with a beam divergence of0.2 degrees will still interfere in the far field. However, in FIG. 60,a 5 degree difference with a beam divergence of 0.2 degrees will notinterfere in the far field even though it may interfere in the nearfield.

Referring to FIGS. 61,62, alternatively, the reflective surface 609 maybe tilted relative to the end view of the element 8 such that the secondcode beam 932 is never generated. This is accomplished by placing a linenormal to the reflective surface out of the plane of incidence for thegrating 12. This occurs because the reflective surface reflects thepassed beam away from the grating 12 and allows the incident andreflected beams to pass the grating without re-introducing them to thegrating 12. In FIG. 61, consider the plane of the page to be the planeof incidence for the grating 12. The normal to the reflective surface906 is pointing somewhere out of the plane of the paper, and is notshown in this view.

Referring to FIG. 62, the view from the end of the grating 12, thereflective surface 906 is tilted an angle θ1 such that the normal line942 is tilted away from the plane of incidence 944 by an angle θ2, sothat the reflected beams 935 and 933 do not intersect with the grating12. Accordingly, this avoids the second code beam 932 from beinggenerated and no interference between the two code beams can occur.Referring to FIG. 63, this can also be accomplished by having theout-of-plane angle of the incident beam 24 be tilted an angle θ2 fromthe line 942 normal to the reflective surface 906.

Referring to FIGS. 64 and 65 a set up for reading the code anddetermining the angle for the reflective surface 906 is shown. Inparticular, a laser source 950 provides a laser beam 952 through aseries of lenses 954 which provides the incident beam 24 to the element8 which is mounted to a reflective plate 956 (e.g., Si-groove plate orother reflective plate). The code beam 935 emerges from the element 8and is reflected off a mirror 957 and is incident on a code reader 958.The plate 956 may be able to pivot or tilt about an axis or point 960 toadjust the angle of incident of the incident beam 24. The device forreading the code may be any of those discussed herein or in thereferenced copending patent applications or any other reader capable ofreading the diffracted optical signal and converting it into a code,such as that described in US patent applications, publication numbers:WO 2004/025559; PCT/US 03/28874 (CV-0038A), WO 2004/024328; PCT/US03/28862 (CV-0042), WO 2004/066210; PCT/US 04/01685 (CV-0054), and WO2005/033681; PCT/US 04/032084 (CV-0092), which are all incorporatedherein by reference in their entirety. However, any type of readercapable of reading the elements 8 may be used.

Referring to FIG. 65, illustrations (a) and (b), the filaments 918 maybe disposed on the reflective plate 956 in various ways. If the plate956 has no grooves and filaments 918 are used as in illustration (a),the filaments 918 may be attached to the plate with hold downs 962. Ifthe plate 956 has grooves 964, the filaments 918 as in illustration (b),the filaments 918 may be held in place by the grooves and an optionaltop plate (not shown). In general, the filaments 918 may be glued ortapes or attached in any fashion to the reflective plate 956. Also, ifthe plate 956 lays substantially flat or horizontal, there is no need tosecure the filaments or beads in grooves or to the plate 956 for basicinterrogation.

In addition, the digital code lends itself naturally to known covert,anti-counterfeit, and/or anti-theft type encoding, authentication, andidentification techniques for items. For example, the code may containan encrypted code that only the manufacturer can read and understandwith the proper decryption. Also, a plurality of beads or elements 8having different codes may be placed in or on a single item and all thecodes would to be read together or in a certain order for them to obtainthe intended tracking, identification or authentication information.Alternatively, one of the codes may be a key to de-encrypt the codes onthe other beads in the same item. Also, the codes may constantly beupdated, e.g., rolling codes, or any combination of private and/orpublic key encryption may be used. Any other use of a bead combinationand/or encryption/decryption techniques may be used if desired. Somenon-limiting examples of digital encryption techniques are described inthe following patents, each of which are incorporated herein byreference in their entirety. RE36,752 Cryptographic authentication oftransmitted messages using pseudorandom numbers 5,952,937 System andmethod of updating communications in a security system 5,940,002Security system with random number remote communication RE36,181Pseudorandom number generation and crytographic authentication 5,783,994Vehicle security system with combined key fob and keypad anti-driveawayprotection 5,757,923 Method of generating secret identification numbers5,696,828 Random number generating system and process based on chaos5,649,014 Pseudorandom composition-based cryptographic authenticationprocess 5,619,575 Pseudorandom composition-based cryptographicauthentication process 5,598,476 Random clock composition-basedcryptographic authentication process and locking system 5,398,284Cryptographic encoding process 5,377,270 Cryptographic authentication oftransmitted messages using pseudorandom numbers 5,363,448 Pseudorandomnumber generation and cryptographic authentication

Also see, Numerical Recipes, The Art of Scientific Computing, by WilliamH. Press, et al, Cambridge University Press; 1986; Basic Methods ofCryptography by Jan C. A. van der Lubbe, et al, Cambridge Univ. Press1998; Applied Cryptography: Protocols, Algorithms, and Source Code in C,by Bruce Schneie, which are incorporated herein by reference in theirentirety. Further, as discussed hereinbefore, the code(s) may containlot or batch numbers, date codes, and/or manufacturer codes. One of theadditional security benefits of using encrypted data is that the itemmanufacturer (e.g., drug company, explosives company, etc) is the onlyone who knows the meaning of the bead codes, so even the bead codemanufacturer will not know what the code represents.

Any of the labeling techniques described herein for labeling items maybe used solely with the encoded elements or encoding technique of thepresent invention or in combination with other labeling, encoding,tracking, identification, authentication, or sorting technology, such asbar codes, RFID, other technologies.

In addition to using the above described techniques with pills or drugsor packages/containers associated therewith, any item being labeled mayuse these same techniques for identification purposes.

Unless otherwise specifically stated herein, the term “microbead” or“bead” is used herein as a label and does not restrict any embodiment orapplication of the present invention to certain dimensions, materialsand/or geometries and is interchangeable with the term “element” asdescribed generally herein.

The dimensions and geometries for any of the embodiments describedherein are merely for illustrative purposes and, as such, any otherdimensions may be used if desired, depending on the application, size,performance, manufacturing requirements, or other factors, in view ofthe teachings herein.

It should be understood that, unless stated otherwise herein, any of thefeatures, characteristics, alternatives or modifications describedregarding a particular embodiment herein may also be applied, used, orincorporated with any other embodiment described herein. Also, thedrawings herein are not drawn to scale.

Although the invention has been described and illustrated with respectto exemplary embodiments thereof, the foregoing and various otheradditions and omissions may be made therein and thereto withoutdeparting from the spirit and scope of the present invention.

1. An optical identification element for identifying a drug, comprising:an optical substrate; at least a portion of said substrate being made ofa substantially single material and having at least one diffractiongrating embedded therein, said grating having a resultant refractiveindex variation within said single material at a grating location; saidgrating providing an output optical signal indicative of a code whenilluminated by an incident light signal propagating in free space; andthe element being at least partially disposed on or within said drug. 2.The apparatus of claim 1, wherein said refractive index variationcomprises at least one refractive index pitch superimposed at saidgrating location.
 3. The apparatus of claim 1, wherein said refractiveindex variation comprises a plurality of refractive index pitchessuperimposed at said grating location.
 4. The apparatus of claim 1,wherein said substrate is made of a material selected from the group:glass, silica, plastic, rubber, and polymer.
 5. The apparatus of claim1, wherein said code comprises at least a predetermined number ofdigital bits, said number being: 3, 5, 7, 9, 10, 12, 14, 16, 18, 20, 24,28, 30, 40, 50, or
 100. 6. The apparatus of claim 1, wherein said codecomprises a plurality of bits, each bit having a corresponding spatiallocation and each bit in said code having a value related to theintensity of said output optical signal at the spatial location of eachbit.
 7. The apparatus of claim 1 wherein said substrate has a lengththat is less than about 1000 microns.
 8. The apparatus of claim 1wherein said substrate has a diameter that is less than about 250microns.
 9. The apparatus of claim 1 wherein at least a portion of saidsubstrate is has a 3-D shape selected from the group: cylinder, sphere,a cube, a pyramid.
 10. The apparatus of claim 1 wherein said substratecomprises a particle or bead.
 11. The apparatus of claim 1 wherein saidsubstrate comprises a filament or thread.
 12. The apparatus of claim 1wherein said drug comprises pharmaceutical products, medical, healthcare products, cosmetics products, and/or the packages or containersthat are supplied therewith.
 13. The apparatus of claim 1 wherein saidcode comprises an encypted code.
 14. The apparatus of claim 1, whereinsaid substrate comprises on or more of the following: a film, anadhesive film, a shrink wrap film, a label, a security label.
 15. A drughaving a optical element disposed therein or thereon, comprising: anoptical substrate; at least a portion of said substrate being made of asubstantially single material and having at least one diffractiongrating embedded therein, said grating having a resultant refractiveindex variation within said single material at a grating location; saidgrating providing an output optical signal indicative of a code whenilluminated by an incident light signal propagating in free space; andsaid code identifying the drug.
 16. A method of reading a code in anoptical identification element that is disposed on or within a drug, theelement having a diffraction grating having a resultant refractivevariation at a grating location, comprising: illuminating said elementwith incident light, said substrate providing an output light signal;and reading said output light signal and detecting a code therefrom. 17.A method for labeling a drug, comprising: obtaining an opticalidentification element having at least one diffraction grating disposedtherein, the grating having a resultant refractive index variation at agrating location; the grating providing an output optical signal whenilluminated by an incident light signal; and the optical output signalbeing indicative of a code; the element being disposed at leastpartially on or within the drug.
 18. The method of claim 19, where thedrug is selected from the group, comprising: large or small pills,capsules, liquid medicine, and powdered medicine.
 19. The method ofclaim 19, wherein said code comprises a digital code indicative ofinformation relating to: identity, type of item, lot number,manufacturer, serial number, date code, or code accuracy.
 20. Theapparatus of claim 1, where the drug is selected from the group,comprising: large or small pills, capsules, liquid medicine, andpowdered medicine.